Chapter 1 VECTOR ALGEBRA

Similar documents
Reference. Vector Analysis Chapter 2

Electromagnetics P5-1. 1) Physical quantities in EM could be scalar (charge, current, energy) or vector (EM fields).

Multiple Integrals. Review of Single Integrals. Planar Area. Volume of Solid of Revolution

Multiple Integrals. Review of Single Integrals. Planar Area. Volume of Solid of Revolution

Chapter 2. Vectors. 2.1 Vectors Scalars and Vectors

(b) Let S 1 : f(x, y, z) = (x a) 2 + (y b) 2 + (z c) 2 = 1, this is a level set in 3D, hence

Higher Checklist (Unit 3) Higher Checklist (Unit 3) Vectors

Analytically, vectors will be represented by lowercase bold-face Latin letters, e.g. a, r, q.

On the diagram below the displacement is represented by the directed line segment OA.

DEFINITION OF ASSOCIATIVE OR DIRECT PRODUCT AND ROTATION OF VECTORS

Physics 3323, Fall 2016 Problem Set 7 due Oct 14, 2016

Chapter 7 Steady Magnetic Field. september 2016 Microwave Laboratory Sogang University

2A1A Vector Algebra and Calculus I

Thomas Whitham Sixth Form

SCHOOL OF ENGINEERING & BUILT ENVIRONMENT. Mathematics

Partial Derivatives. Limits. For a single variable function f (x), the limit lim

The Algebra (al-jabr) of Matrices

Chapter 4 Contravariance, Covariance, and Spacetime Diagrams

ragsdale (zdr82) HW2 ditmire (58335) 1

Electromagnetism Answers to Problem Set 10 Spring 2006

Candidates must show on each answer book the type of calculator used.

INTRODUCTION TO LINEAR ALGEBRA

Eigen Values and Eigen Vectors of a given matrix

2. VECTORS AND MATRICES IN 3 DIMENSIONS

Computer Graphics (CS 4731) Lecture 7: Linear Algebra for Graphics (Points, Scalars, Vectors)

THE DISCRIMINANT & ITS APPLICATIONS

Lesson Notes: Week 40-Vectors

Problem 1. Solution: a) The coordinate of a point on the disc is given by r r cos,sin,0. The potential at P is then given by. r z 2 rcos 2 rsin 2

10.5. ; 43. The points of intersection of the cardioid r 1 sin and. ; Graph the curve and find its length. CONIC SECTIONS

Phys 4321 Final Exam December 14, 2009

Theoretische Physik 2: Elektrodynamik (Prof. A.-S. Smith) Home assignment 4

MATRICES AND VECTORS SPACE

THREE-DIMENSIONAL KINEMATICS OF RIGID BODIES

Things to Memorize: A Partial List. January 27, 2017

This final is a three hour open book, open notes exam. Do all four problems.

JUST THE MATHS SLIDES NUMBER INTEGRATION APPLICATIONS 12 (Second moments of an area (B)) A.J.Hobson

Lecture 13 - Linking E, ϕ, and ρ

Plane curvilinear motion is the motion of a particle along a curved path which lies in a single plane.

APPLICATIONS OF DEFINITE INTEGRALS

P 1 (x 1, y 1 ) is given by,.

JUST THE MATHS UNIT NUMBER INTEGRATION APPLICATIONS 12 (Second moments of an area (B)) A.J.Hobson

KINEMATICS OF RIGID BODIES

Plane curvilinear motion is the motion of a particle along a curved path which lies in a single plane.

PROPERTIES OF AREAS In general, and for an irregular shape, the definition of the centroid at position ( x, y) is given by

Conducting Ellipsoid and Circular Disk

CAPACITORS AND DIELECTRICS

Point Lattices: Bravais Lattices

Time : 3 hours 03 - Mathematics - March 2007 Marks : 100 Pg - 1 S E CT I O N - A

CHAPTER 6 Introduction to Vectors

CBSE-XII-2015 EXAMINATION. Section A. 1. Find the sum of the order and the degree of the following differential equation : = 0

Algebra Of Matrices & Determinants

50. Use symmetry to evaluate xx D is the region bounded by the square with vertices 5, Prove Property 11. y y CAS

MATH 13 FINAL STUDY GUIDE, WINTER 2012

Basics of space and vectors. Points and distance. Vectors

Chapter 3. Vector Spaces

Final Exam Solutions, MAC 3474 Calculus 3 Honors, Fall 2018

Maths in Motion. Theo de Haan. Order now: 29,95 euro

Phys 6321 Final Exam - Solutions May 3, 2013

Physics 2135 Exam 1 February 14, 2017

Jackson 2.7 Homework Problem Solution Dr. Christopher S. Baird University of Massachusetts Lowell

4 VECTORS. 4.0 Introduction. Objectives. Activity 1

SECTION 9-4 Translation of Axes

A1 Vector Algebra and Calculus

STRAND J: TRANSFORMATIONS, VECTORS and MATRICES

5.2 Volumes: Disks and Washers

Operations with Polynomials

Distributed Forces: Centroids and Centers of Gravity

3. Vectors. Home Page. Title Page. Page 2 of 37. Go Back. Full Screen. Close. Quit

III. Vector data. First, create a unit circle which presents the margin of the stereonet. tan. sin. r=1. cos

Method of Localisation and Controlled Ejection of Swarms of Likely Charged Particles

13.4 Work done by Constant Forces

Chapter 9. Arc Length and Surface Area

Homework Assignment 6 Solution Set

Partial Differential Equations

Homework Assignment 3 Solution Set

Math 6A Notes. Written by Victoria Kala SH 6432u Office Hours: R 12:30 1:30pm Last updated 6/1/2016

Gravitation (Symon Chapter Six)

10 Vector Integral Calculus

Some Methods in the Calculus of Variations

Motion of Electrons in Electric and Magnetic Fields & Measurement of the Charge to Mass Ratio of Electrons

Chapter 6 Electrostatic Boundary Value Problems. Dr. Talal Skaik

Vectors and the Geometry of Space

Week 10: Line Integrals

ARITHMETIC OPERATIONS. The real numbers have the following properties: a b c ab ac

Mathematics. Area under Curve.

Today in Physics 122: work, energy and potential in electrostatics

1.2 What is a vector? (Section 2.2) Two properties (attributes) of a vector are and.

LINEAR ALGEBRA APPLIED

3. Vectors. Vectors: quantities which indicate both magnitude and direction. Examples: displacemement, velocity, acceleration

Optimization Lecture 1 Review of Differential Calculus for Functions of Single Variable.

KINEMATICS OF RIGID BODIES

Physics Jonathan Dowling. Lecture 9 FIRST MIDTERM REVIEW

Physics Graduate Prelim exam

Problem Set 3 Solutions

CONIC SECTIONS. Chapter 11

JUST THE MATHS UNIT NUMBER INTEGRATION APPLICATIONS 8 (First moments of a volume) A.J.Hobson

Magnetic forces on a moving charge. EE Lecture 26. Lorentz Force Law and forces on currents. Laws of magnetostatics

Electromagnetic Potentials and Topics for Circuits and Systems

R(3, 8) P( 3, 0) Q( 2, 2) S(5, 3) Q(2, 32) P(0, 8) Higher Mathematics Objective Test Practice Book. 1 The diagram shows a sketch of part of

Chapter 5 Determinants

Transcription:

Chpter 1 VECTOR LGEBR

INTRODUCTION: Electromgnetics (EM) m be regrded s the stud of the interctions between electric chrges t rest nd in motion. Electromgnetics is brnch of phsics or electricl engineering in which electric nd mgnetic phenomen re studied.

PPLICTION EM principles find ppliction in vrious disciplines such s; micowves,ntenns electric mchines stellite communictios Bioelectromgnetics plsms,nucler reserch,fiberoptics

Sclr nd Vectors sclr is quntit tht hs onl mgnitude. Quntities such s time,mss,distnce,temperture,entrop h,electric potentil.

VECTORS vector is quntit tht hs both mgnitude nd direction. Vector quntities include velocit,force,displcement nd electric field intensit.

UNIT VECTOR vector hs both mgnitude nd direction. The mgnitude of is sclr written s or unit vector long is defined s vector whose mgnitude is unit nd its direction is long, tht is;

UNIT VECTOR n

vector in Crte coordintes m be represented s; (,, ) + +

VECTOR DDITION & SUBTRCTION Two vectors nd B cn be dded together to give nother vector C C + B Let (,, ) nd B(B, B,B ) C ( + B ) + ( + B ) + ( + B )

Vector subtrction is similrl crried out s; D B + (-B) D ( -B ) + ( -B ) + ( -B )

Vector lgebr

Vector lgebr ddition ssocitive lw +(B+C) (+B)+C commuttive lw +B B+ multipliction b sclr B B distributive lw ( B+C) B + C

POSITION ND DISTNCE VECTOR point P in Crte coordintes m be represented b (,,). The position vector r p (rdius vector)of point P is s the directed distnce from the origin O to P; i.e., r p OP + +

P (3,4,5) 0 Z5 X3 Y4 POSITION VECTOR OP3 + 4 + 5

Distnce Vector P r PQ r p Q 0 r Q r PQ r Q -r p

Emples: If 10 4 + 6 nd B2 +. Find: () The components of long (b) The mgnitude of 3-B (c) unit vector long + 2B

Solution: () The component of long is -4 (b) 3-B 3(10,-4,6)-(2,1,0) (30,-12,18)-(2,1,0) (28,-13,18) Hence;

3 B 28 2 + ( ) 2 13 + ( 18) 2 35.74

( c ) Let C + 2B (10,-4,6) + (4,2,0) (14,-2,6) unit vector long C is c C C 14 2 ( 14, 2,6 ) + ( ) 2 2 + 6 2

Emples:2 Points P nd Q re locted t (0,2,4) nd (-3,1,5).Clculte () The position vector P (b) The distnce vector from P to Q (c) The distnce between P nd Q (d) vector prllel to PQ with mgnitud of 10

Solution 2 () r p 0 + 2 + 4 (b) r PQ r Q r P (-3,1,5)-(0,2,4)(-3,- 1,1) (c) Since r PQ is the distnce vector from P to Q,the distnce between P nd Q is the mgnitude of this vector;tht is, d r PQ 9 + 1+ 1 3.317

(d) Let the required vector be,then Where 10 is the mgnitude of.since is prllel to PQ, it must hve the sme unit vector s r PQ or r QP. Hence,

-9.045-3.015 +3.015

VECTOR MULTIPLICTION When two vector nd B re multiplied,the result is either sclr or vector depending on how the re multiplied. Thus there re two tpes of vector multipliction: 1. Sclr (or dot) product:.b 2. Vector(or Cross)product:XB

DOT PRODUCT The dot product of two vector nd B,written.B is defined geometricll s the product of the mgnitudes of nd B nd the ine of the ngle between them..b B B

The Vector Field Emple The Dot product.b B B B in the direction of You need to normlie before the dot product.

B Where is the smller ngle between nd B. The result of.b is clled either the sclr product. Let (,, ) nd B (B,B,B ).B B + B + B

Two vectors nd B re sid to be orthogonl (or perpendiculr) with ech other if.b0 Note tht dot product obes the following; (i) Commuttive Lw;.BB. (ii) Distributive lw :.(B+C).B +.C. 2

(iii) lso note tht... 0... 1

Cross Product The cross product of two vector nd B,written X B, is vector quntit whose mgnitude is the re of the prllelopiped formed b nd B B B

The Cross Product B N B B B Emple B B B 2 : 3 B 1 : 4 2 5 B 13 14 16

The cross product hs the bsic following properties: (i) It is not commuttive: B B (ii) It is not ssocitive; ( B C )( B ) C (iii) It is distributive (B+C)XB +XC

(iv) 0 lso note tht;,,

Cross Product ug clic permuttion. - - -

Emple:1 Determine the dot product nd cross product of the following vectors. 2 + 3 4 B -1 5 + 6

SOLUTION The dot product is.b (2)(-1) + (3) (-5) + (-4)(6) -41 The Cross Product B is B [ (3)(6) (-4)(-5)] + [(-4)(-1) (2)(6)] + [(2)(-5) (3)(-1)] -2-8 -7

lterntivel B - B B 2 +8 + 7

Sclr Triple Product Given three vector,b nd C.(BC)B.(C)C.(B) If (,, ), B(B,B,B ) nd C(C,C,C ).(BC) B B B Z C C C

Vector Triple product For vectors,b, nd C, we define the vector triple product s (BC)B(.C)-C(.B) It should be noted tht (.B)C(B.C) But (.B)CC(.B)

Coordinte Sstems nd Trnsformtion. Crte Coordintes (,,) Circulr Clindricl Coordintes ( ρ,, ) Sphericl Coordintes ( r,, )

Crte Coordinte Consists of three mutull orthogonl es,,, nd point in spce is denoted s P( 1, 1, 1 ). The loction of the point is defined b the intersection of three plnes.

Z P( 1, 1, 1 ) Z 1 1 1 + +

The Crte Coordinte Sstem

The differentil surfces in crte coordintes Differentil Surfces ds dd ds dd ds dd ds dd d d d ds dd ds dd

Crte Coordintes (,,) The Rnges of the coordinte vribles,, re;

Vector Components nd Unit Vectors

The Clindricl Coordintes Sstem. Form b three surfces One is plne for constnt, 1 The net surfce is clinder centered on the is of rdius ρ The third surfce is plne perpendiculr to the plne nd rotte bout the is b ngle Unit vector ρ,, point in the direction of increg coordinte vlue.

Circulr Clindricl Coordinte Sstem ρ dρ ρ d d 1 - Unit Vector vr with The coordinte Since direction chnges 2 Dot Product ρ d d ρ dρ d d

Clindricl coordinte sstem + 1 2 2 tn ρ ϕ ρ ρ ρ ρ

Z ρ S C Q D B d ρd dρ ρ

ρ d ρ ρ d

Differentil norml res in clindricl coordintes. ρd ρ d d ρ d d ρ ρ d

In Clindricl Coordintes,differentil elements cn be found s follows; (1) Differentil displcement is given b di dρ + ρd + ρ d (2) Differentil norml re is given b ds ρ d d ρ dρd ρddρ

(3) Differentil volume is given b dv ρ d ρ d d

Circulr Clindricl Coordinte Sstem ρ () ρ () Dot Product ρ 2 + 2 ρ 0 tn + + ρ ρ + + ρ ρ ρ ( + + ) ρ ρ + ρ ρ () ρ ( ) 1 ( + + ) + () () ( + + ) ρ 0

Emple: () Determine the volume enclosed b clinder of rdius ρ nd the length L s well s the surfce re of tht volume. (b) The surfce re?

Solution: To determine the volume enclosed we integrte; V v dv ρ ρ 0 πρ 2 2π L L 0 0 ρdrdd 14243 dv

2π L 2π ρ 2π ρ S 0 0 ρ d d 14243 4 Sides + 0ρ 0 rd dr 14243 bottom + 0ρ 0 rd top dr 14243 2πρL + 2πρ 2

Sphericl Coordintes point P cn be represented s ( r,, ) in this coordinte sstem vector in sphericl coordintes is written s or ( r,, ) + + r r Where, nd r re unit vectors long -direction. r,, nd

The Sphericl Coordinte Sstem ( ) r ( ) ( ()) r r ( ) r 2 + 2 + 2 r 0 2 + 2 + 2 0 180 tn

+ + + + r 1 2 2 2 1 2 2 2 tn Sphericl coordinte sstem r ϕ r r r

The Sphericl Coordinte Sstem ( ) r ( ) ( ()) r r ( ) rdr d ( ) r ( ) r 2 dr d d d r 2 ( ) dr d d

The rnges of vribles re; 0 r 0 π 0 2 π

r d dr rd r d d

Z r d r rd Differentil rc length for constnt

Z r d r r d rd Differentil rc length for constnt

Differentil norml res in sphericl coordintes; r d r r d rd dr rd () (b) (C) dr

(1) The differentil displcement is dl dr + rd + r r d (2) The Sphericl Coordinte Sstem ds r 2 r rdrd d drd d r

The differentil volume is dv r 2 drd d

Emple: Determine the volume enclosed b sphere of rdius r

Solution: v dv v r r 0 π 0 2π 0 r 2 drd d 4 3 π r 2

The reltionships between the vribles (,,) of the Crte Coordinte Sstem. P (,,)P ( ρ,, ) ρ ρ ρ

The mgnitude of is; 2 2 ρ + + 2 The reltionship between,, nd re obtined geometricll from, ρ, ρ + ρ

+ + Let ρ ρ convert to crte coordinte. + +. ( + + ) ρ ρ ρ ( ) ( ) + + ) ρ (

ρ ρ ρ π 2 + ρ

. ( + + ) ρ ρ ( ) ( ) + + ) ρ ρ ( + ρ Z Z

r 0 0 0 0 0

Performing dot-product ρ ρ

Clinder to Crte Crte to Clinder ρ ρ 2 + 2 ρ tn 1

EXMPLES:4 Given point P(-2,6,3) nd Vector + (+),epress P nd in clindricl coordintes. Evlute t P in Crte nd Clindricl sstems.

Solution: t Point P: -2, 6, 3 Hence, ρ 2 + 4+ 36 2 6.32 6 2 1 1 tn tn 108.43 0 Z3

Thus, P(-2,6,3)P(6.32,108.43 0,3) In the crte stem, t P is 6 + For vector,, + 0, Hence the clindricl sstem + 0 1 0 0 0 0 ρ

ρ + ( + ) + ( + ) But ρ, ρ

ρ ρ 008 6. 0.9487 40 38 40 6 ( ) [ ] ( ) [ ] ρ ρ ρ ρ ρ ρ ),, ( 2 + + + + + 40 6 40 2, 2 6 tn 40 ρ Hence P t

Crte Coordintes to Sphericl Coordintes Sstem Z ρ r P(,, ) P( r,, ) P( ρ,, ) r r ρ ρ ρ

r + + + +

In Mtri form,the ),, ( ),, ( r r r r r r 0 ),, ( ),, ( 0 r r tion Trnsform Inverse The

Dot Product of unit vectors in sphericl nd crte coordintes sstem. r 0

2 2 r + + 2 tn 1 2 + 2 tn 1

r r r

Emple: Evlute t P in the sphericl sstem s in Emple 4

In the sphericl sstem ) ( ) ( ) ( or r + + + + + + + 0 0 r

END